Problem 24

Question

Super fluids The 1996 Nobel Prize in Physics was awarded to Douglas Osheroff, Robert Richardson, and David Lee for discovering super-fluidity (apparently frictionless flow) in "He. When \(^{3} \mathrm{He}\) is cooled to \(2.7 \mathrm{mK}\), the liquid settles into an ordered super-fluid state. What is the predicted sign of the entropy change for the conversion of liquid ' He into its super-fluid state?

Step-by-Step Solution

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Answer
The sign of entropy change for the conversion of liquid helium into its superfluid state is negative, indicating a decrease in entropy. This is because the system becomes more ordered during the transition and loses heat to its surroundings.
1Step 1: Understand entropy change
Entropy change, denoted by \(\Delta S\), is a measure of the change in the number of microstates in a system. If a system becomes more ordered, as it does when it transitions from a liquid state to a superfluid state, the number of possible microstates the particles can occupy decreases, resulting in a negative entropy change. Since entropy change is linked to the heat transfer and temperature, we can also check the sign using the formula: $$\Delta S = \frac{q}{T}$$ where \(q\) represents heat transfer and \(T\) is the temperature in Kelvin.
2Step 2: Analyze heat transfer during the transition of liquid helium to superfluid
As helium is cooled to \(2.7\,\text{mK}\) to undergo the phase transition, it means that the system is losing heat to the surroundings, hence \(q\) is negative.
3Step 3: Analyze temperature sign during the process
The given temperature is \(2.7\,\text{mK}\). Since a temperature can never be negative, the value of \(T\) is positive.
4Step 4: Determine the sign of entropy change using the formula
Using the formula \(\Delta S = \frac{q}{T}\), since \(q\) is negative and \(T\) is positive, the sign of \(\Delta S\) will be negative, indicating a decrease in entropy. So, the predicted sign of the entropy change for the conversion of liquid helium into its superfluid state is negative.

Key Concepts

Entropy ChangePhase TransitionHelium-3
Entropy Change
When we talk about entropy change in the context of superfluidity, we are referring to how "chaotic" or "ordered" the system's particles become. Entropy, in simple terms, is a measure of disorder. If a system becomes more organized—like when liquid helium transitions into a superfluid—it means there's less randomness or fewer microstates available.
This implies a decrease in entropy. In mathematical terms, the entropy change represented by \(\Delta S = \frac{q}{T}\)can be used to determine the behavior of a system during a transition.
In this formula:
  • \(q\) represents the amount of heat transfer—whether the system absorbs or releases heat.
  • \(T\) is the temperature in Kelvin, ensuring it remains positive.
When we go from a liquid to a superfluid state, the heat is released to the environment (\(q\) is negative), causing \(\Delta S\)to be negative, as the particles settle into a more orderly state.
Phase Transition
Phase transitions happen when a substance changes from one state of matter to another, like liquid to gas, or in this case, liquid helium-3 turning into a superfluid.
Superfluidity is a remarkable state where helium flows without any internal friction, resulting in incredibly unique properties. For such a phase change to occur, conditions must be just right—typically at extremely low temperatures.
For helium-3, this occurs around \(2.7 \, \text{mK}\).
During this transition:
  • Energy in the form of heat is released as the system becomes more ordered.
  • The molecular motion changes, allowing the particles to condense into a super-ordered phase.
While most transitions occur with heat absorption, the superfluid transition involves heat release, aligning with the idea of decreasing entropy.
Helium-3
Helium-3 \(\left(^{3}\mathrm{He}\right)\) is a rare isotope of helium that acts quite differently compared to the more common helium-4. One of the most interesting behaviors of helium-3 is its ability to become a superfluid very close to absolute zero. This superfluid state arises at approximately \(2.7 \mathrm{mK}\).
Its uniqueness comes from its atomic structure:
  • Helium-3 atoms are "fermions," meaning they obey Fermi-Dirac statistics.
  • At low temperatures, they pair up to form "bosons," which can occupy the same quantum state—this is crucial for superfluidity.
Understanding helium-3's properties helps in studying quantum mechanics and low-temperature physics. Its transition into a superfluid state at such low temperatures has fascinating implications for both theoretical and applied sciences, offering insights into the quantum world and superfluid behavior.